Doped fiber amplifier using bidirectional pumping with pump lights having different frequencies

ABSTRACT

A doped fiber amplifier which provides bidirectional pumping to amplify a signal light, and reduces instability of gain caused by the bidirectional pumping. The doped fiber amplifier includes a rare earth element doped optical fiber, a first light source and a second light source. The optical fiber has first and second ends, with the signal light propagating through the optical fiber from the first end to the second end. The first light source provides pump light which propagates in the optical fiber from the first end to the second end and is at a first wavelength. The second light source provides pump light which propagates in the optical fiber from the second end to the first end and is at a second wavelength. The first wavelength is different from the second wavelength. The pump light provided by the first and second light sources causes the signal light to be amplified as the signal light propagates through the optical fiber.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is based on, and claims priority to, Japanese patentapplication number 08-037657, filed on Feb. 26, 1996, in Japan, andwhich is incorporated herein by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an optical amplifier, such as a dopedfiber amplifier, using bidirectional pumping to amplify a signal lightpropagating through a doped optical fiber. More particularly, thepresent invention relates the relationship between the wavelengths ofthe pump light used for bidirectional pumping, and to the control of thepump light to adjust tilt gain of the doped fiber amplifier.

2. Description of the Related Art

There is increasing demand for communication systems, such as multimedianetworks, which can provide high speed transmission and large bandwidth.Moreover, optical communication systems which use wavelength divisionmultiplexing (WDM) promise to provide such high speed transmission andlarge bandwidth.

In optical communication systems which use WDM, a rare earth elementdoped fiber amplifier is typically used to amplify optical signals sincethis type of doped fiber amplifier has a relatively wide gain band. Awide gain band is generally required to amplify all the channels whichmay be included in a wavelength division multiplexed signal light.

In such a rare earth element doped fiber amplifier, either forwardpumping or backward pumping can be used to amplify signal light. Withforward pumping, a light source produces pump light which propagatesthrough the fiber in the same direction as the signal light propagates.The forward travelling pump light interacts with the rare earth elementdoped fiber to amplify the signal light. With backward pumping, a lightsource produces pump light which propagates through the fiber in theopposite direction as the signal light propagates. The backwardtravelling pump light interacts with the rare earth element doped fiberto amplify the signal light. With bidirectional pumping, both forwardand backward pump light are provided in the fiber, so that the signallight is amplified by both the forward and backward pump light.

Unfortunately, with bidirectional pumping, one of the light sourcesproviding pump light will be influenced by pump light provided by theother light source. For example, a light source providing the forwardpump light may be influenced by the backward pump light. Similarly, alight source providing the backward pump light may be influenced by theforward pump light. As a result, the gain of the doped fiber amplifierbecomes instable.

SUMMARY OF THE INVENTION

Accordingly, it is an object of the present invention to provide a dopedfiber amplifier which uses bidirectional pumping and provides a stablegain.

It is an additional object of the present invention to provide a dopedfiber amplifier which uses bidirectional pumping, wherein a relationshipbetween the wavelength of forward pump light and the wavelength ofbackward pump light provides a stable gain.

Objects of the present invention are achieved by providing an apparatus,such as a doped fiber amplifier, for amplifying a signal light. Theapparatus includes an optical fiber, a first light source and a secondlight source. The optical fiber has first and second ends, with thesignal light propagating through the optical fiber from the first end tothe second end. The first light source provides pump light whichpropagates in the optical fiber from the first end to the second end andis at a first wavelength. The second light source provides pump lightwhich propagates in the optical fiber from the second end to the firstend and is at a second wavelength. The first wavelength is differentfrom the second wavelength. The pump light provided by the first andsecond light sources causes the signal light to be amplified as thesignal light propagates through the optical fiber.

Objects of the present invention are also achieved by providing a gaintilt control unit which monitors amplified spontaneous emission (ASE) inthe optical fiber, determines a gain tilt of the apparatus from themonitored ASE, and controls the power of the pump light produced by thefirst light source and/or the power of the pump light produced by thesecond light source, to control the gain tilt. Preferably, the tilt gaincontrol unit controls the tilt gain to be constant.

Objects of the present invention are also achieved by providing anapparatus for amplifying a signal light, wherein the apparatus includesan optical fiber, a light source and a gain tilt control unit. Thesignal light propagates through the optical fiber. The light sourceprovides pump light which propagates in the optical fiber and causes thesignal light to be amplified as the signal light propagates through theoptical fiber. The gain tilt control unit monitors amplified spontaneousemission (ASE) in the optical fiber, determines a gain tilt of theapparatus from the monitored ASE, and controls the power of the pumplight produced by the light source to control the gain tilt.

Objects of the present invention are also achieved by providing a methodfor amplifying a signal light propagating through an optical fiber. Themethod includes the steps of (a) propagating the signal light throughthe optical fiber from a first end to a second end of the optical fiber,(b) propagating first pump light at a first wavelength in the opticalfiber from the first end to the second end so that the first pump lightcauses the signal light to be amplified as the signal light propagatesthrough the optical fiber, and (c) propagating second pump light at asecond wavelength in the optical fiber from the second end to the firstend so that the second pump light causes the signal light to beamplified as the signal light propagates through the optical fiber, thefirst wavelength being a different wavelength than the secondwavelength.

Additional objects and advantages of the invention will be set forth inpart in the description which follows, and, in part, will be obviousfrom the description, or may be learned by practice of the invention.

BRIEF DESCRIPTION OF THE DRAWINGS

These and other objects and advantages of the invention will becomeapparent and more readily appreciated from the following description ofthe preferred embodiments, taken in conjunction with the accompanyingdrawings, of which:

FIG. 1 is a diagram illustrating a doped fiber amplifier, according toan embodiment of the present invention.

FIG. 2 is a graph illustrating characteristics of a reflection typeoptical device, according to an embodiment of the present invention.

FIGS. 3(A) and 3(B) are graphs illustrating the spectra of a pump lightsource, according to embodiments of the present invention.

FIGS. 4(A) and 4(B) are graphs illustrating instability of gain of adoped fiber amplifier.

FIG. 5 is a graph illustrating stability of gain of a doped fiberamplifier, according to embodiments of the present invention.

FIG. 6 is a diagram illustrating a doped fiber amplifier, according toan additional embodiment of the present invention.

FIG. 7 is a graph illustrating wavelength characteristics of gain andnoise figure.

FIG. 8 is a graph illustrating gain tilt of a doped fiber amplifier.

FIG. 9 is a diagram illustrating a doped fiber amplifier, according to afurther embodiment of the present invention.

FIG. 10 a diagram illustrating a control circuit as illustrated in FIG.9, according to an embodiment of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Reference will now be made in detail to the preferred embodiments of thepresent invention, examples of which are illustrated in the accompanyingdrawings, wherein like reference numerals refer to the same or similarelements throughout.

FIG. 1 is a diagram illustrating a doped fiber amplifier, according toan embodiment of the present invention. Referring now to FIG. 1, thedoped fiber amplifier includes a doped fiber 2 having a first end 2A anda second end 2B. Signal light propagates in a propagation direction indoped fiber 2 from first end 2A to second end 2B. Thus, first end 2A ofdoped fiber 2 corresponds to an upstream side of the propagationdirection, and second end 2B corresponds to a downstream side of thepropagation direction. Doped fiber 2 is doped with a rare earth element.Selection of an appropriate rare earth element depends, in part, on thewavelength of the signal light. In the following description, it isassumed that the signal light falls within a 1.55 μm band, and thatdoped fiber 2 is doped with the rare-earth element erbium (Er) sinceerbium is a preferable dopant for signal light in the 1.55 μm band.

A WDM optical coupler 4 connects a pump light source 8 to first end 2Aof doped fiber 2, and a WDM optical coupler 6 connects a pump lightsource 10 to second end 2B of doped fiber 2. Pump light sources 8 and 10each provide pump light in a 0.98 μm band, since pump light in a 0.98 μmband is ideally suited to amplify a signal light which is in a 1.55 μmband and is propagating in an erbium doped fiber.

Optical coupler 4 has ports 4A, 4B, 4C, and 4D. Port 4D is terminated byan antireflection coating. Signal light having a wavelength in a 1.55 μmband is supplied to port 4A and is output from port 4C to first end 2Aof doped fiber 2. Pump light having a wavelength in a 0.98 μm band issupplied to port 4B from pump light source 8 and is output from port 4Cto first end 2A of doped fiber 2.

Similarly, optical coupler 6 has ports 6A, 6B, 6C, and 6D. Port 6B isterminated by an antireflection coating. Signal light having awavelength in a 1.55 μm band is supplied to port 6A from doped fiber 2and is output from port 6C. Pump light having a wavelength in awavelength in a 0.98 μm band is supplied to port 6D from pump lightsource 10 and is output from port 6A to second end of doped fiber 2.

Pump light source 8 includes a laser diode 12 operating in a wavelengthband of 0.98 μm and a reflection type optical device 14 provided betweenlaser diode 12 and port 4B of optical coupler 4. Laser diode 12 issupplied with a direct-current or controlled drive current (biascurrent) from a drive circuit 16.

Similarly, pump light source 10 includes a laser diode 18 operating in awavelength band of 0.98 μm and a reflection type optical device 20provided between laser diode 18 and port 6D of optical coupler 6. Laserdiode 18 is supplied with a direct-current or controlled drive currentfrom a drive circuit 22.

Signal light is supplied through an optical isolator 24 to port 4A ofoptical coupler 4. Pump lights provided by pump light source 8 and pumplight source 10 cause the signal light to be amplified as the signallight propagates through doped fiber 2. The amplified signal light isoutput from port 6C of optical coupler 6 and passes through an opticalisolator 26.

FIG. 2 is a graph illustrating characteristics of a reflection typeoptical device, according to an embodiment of the present invention.More specifically, referring now to FIG. 2, curve 28 illustrates thecharacteristics of reflection type optical device 14, and curve 30illustrates the characteristics of reflection type optical device 20. InFIG. 2, the vertical axis represents reflectivity (%) and the horizontalaxis represents wavelength (nm).

As illustrated by curve 28, reflection type optical device 14 has aselectivity of wavelength in a narrow band having a center wavelengthλ₁. Similarly, as illustrated by curve 30, reflection type opticaldevice 20 has a selectivity of wavelength in a narrow band having acenter wavelength λ₂ (λ₁ ≠λ₂).

The wavelengths λ₁ and λ₂ fall within a 0.98 μm band selected from 0.98μm bands used as pump bands for an erbium doped fiber (EDF). A detuningquantity (|λ₁ -λ₂ |) is preferably greater than or equal to 5 nm. WhileFIG. 2 shows that the wavelength λ₂ is shifted from the wavelength λ₁ tothe longer wavelength side, the side of shifting of the wavelengths λ₁and λ₂ from each other is arbitrary.

FIGS. 3(A) and 3(B) are graphs illustrating spectra of a pump lightsource, such as pump light sources 8 and 10, according to embodiments ofthe present invention. For example, FIG. 3(A) illustrates the spectrumof light output from laser diode 12 of pump light source 8, and FIG.3(B) illustrates the spectrum of light output from reflection typeoptical device 14.

As illustrated in FIG. 3 (A), the light output from laser diode 12 has arelatively wide spectrum. As illustrated in FIG. 3(B), the light outputfrom reflection type optical device 14 and supplied to doped fiber 2 hasa relatively narrow spectrum. Thus, reflection type optical device 14functions to narrow to spectrum of light output from laser diode 12.

Reflection type optical devices 14 and 20 can be, for example, a Braggreflection grating fiber or an interference optical film, such as adielectric multilayer film.

FIGS. 4(A) and 4(B) are graphs illustrating instability of gain of adoped fiber amplifier. In FIGS. 4(A) and 4(B), a solid line curve 29represents the relation between total output power (dBm) of a dopedfiber amplifier and drive current (mA) of a laser diode providing pumplight, and a broken line curve 31 represents the relation between peakwavelength (nm) of the spectrum and drive current (mA).

More specifically, FIG. 4(A) shows characteristics of the doped fiberamplifier illustrated in FIG. 1, in the case that reflection typeoptical devices 14 and 20 have been removed. That is, FIG. 4(A) showsmeasured changes in the total output power and the peak wavelength whena constant drive current is supplied to laser diode 12 for forwardpumping (full pumping) and a drive current supplied to laser diode 18for backward pumping is changed. As can be seen from FIG. 4(A), both thetotal output power and the peak wavelength change discontinuously withan increase in the drive current.

Such instability of gain is due to the fact that the spectrum of pumplights output from laser diodes 12 and 18 is wide, as shown in FIG.3(A), and thereby influence each other. More specifically, after theforward pump light supplied from laser diode 12 to doped fiber 2contributes to optical amplification, a residual portion of the forwardpump light is supplied through optical coupler 6 to pump light source10. This residual portion causes the oscillation of laser diodes 18 tobecome instable. Similarly, after the backward pump light supplied fromlaser diode 18 to doped fiber 2 contributes to optical amplification, aresidual portion of the backward pump light is supplied through opticalcoupler 4 to pump light source 8. This residual portion causes theoscillation of laser diode 12 to become instable.

FIG. 4(B) shows characteristics of the doped fiber amplifier illustratedin FIG. 1, including reflection type optical devices 14 and 20, andwhere the center wavelength of reflection type optical device 14 andcenter wavelength of reflection type optical device 20 are coincidentwith each other. Specifically, both the wavelength of the forward pumplight and the wavelength of the backward pump light are set to 975.0 nm.

FIG. 4(B) shows changes in the total output power and the peakwavelength when full pumping is maintained by laser diode 12 and thedrive current supplied to laser diode 18 is changed. As can be seen fromFIG. 4(B), when the drive current exceeds 50 mA, oscillation at awavelength of 1020 nm occurs from the interaction between pump lightsources 8 and 10, thereby causing a reduction in pumping efficiency.

Thus, in the case that the spectrum of the forward pump light and thespectrum of the backward pump light are narrowed, and the wavelengths ofthe forward pump light and the backward pump light are coincident witheach other, the gain experiences relatively high instability.

FIG. 5 is a graph illustrating stability of gain of the doped fiberamplifier illustrated in FIG. 1, where the wavelength of the forwardpump light is set to 980.0 nm, and the wavelength of the backward pumplight is set to 975.0 nm. More specifically, FIG. 5 shows changes in thetotal output power and the peak wavelength when full pumping ismaintained by laser diode 12 and the drive current supplied to laserdiode 18 is changed.

As can be seen from FIG. 5, the total output power increasescontinuously with an increase in the drive current, thereby providing astable gain. Thus, by making the wavelength of the forward pump lightand the wavelength of the backward pump light different from each other,the interaction between two pump light sources 8 and 10 is suppressedand the gain is stabilized.

FIG. 6 is a diagram illustrating a doped fiber amplifier, according toan additional embodiment of the present invention. Referring now to FIG.6, distributed-feedback (DFB) type laser diodes (LD) 8' and 10' are usedinstead of pump light sources 8 (see FIG. 1) and 10 (see FIG. 1). DFBlaser diode 8' operates in a single mode in a wavelength band having acenter wavelength λ₁, to provide forward pumping. DFB laser diode 10'operates in a single mode in a wavelength band having a centerwavelength λ₂, to provide backward pumping. As previously described, thewavelengths λ₁ and λ₂ fall within a pump band of 0.98 μm, and aredifferent from each other.

As illustrated in FIG. 6, bidirectional pumping is performed by twolaser diodes each operating in a single mode. Accordingly, the gain ofthe doped fiber amplifier can be stabilized without using reflectiontype optical devices.

FIG. 7 is a graph illustrating wavelength characteristics of gain andnoise figure of a doped fiber amplifier as illustrated in FIGS. 1 and 6.In FIG. 7, the vertical axes represent gain (dB) and noise figure (dB),and the horizontal axis represents wavelength (nm) of pump light inforward pumping or backward pumping. Thus, curve 33 represents a noisefigure curve, and curve 35 represents a gain curve.

Referring now to FIG. 7, in an erbium doped fiber (EDF), such as dopedfiber 2, a wavelength λ_(minNF) providing a minimum noise figure is 980nm, and wavelengths λ_(maxG) providing a maximum gain are 975 nm and 985nm. Further, a preferable pump band of 0.98 μm that can provide asufficient gain for actual use ranges from 965 nm to 995 nm.

Preferably, the wavelength λ₁ of the forward pump light is set equal toλ_(minNF) so that a low noise figure is achieved at the upstream side ofdoped fiber 2 where signal light has not yet been highly amplified. Thatis, the wavelength λ₁ of the forward pump light is set substantiallyequal to 980 nm, and the wavelength λ₂ of the backward pump light is setto fall substantially within the range of 965 nm to 995 nm, therebyobtaining a doped fiber amplifier having a stable gain and relativelylow noise.

Therefore, when the wavelength λ₁ of the forward pump light is set equalto λ_(minNF) and the wavelength λ₂ of the backward pump light is setequal to λ_(maxG), it is possible to provide a doped fiber amplifierhaving a stable gain, a low noise, and a high output. Specifically, inthis case, the wavelength λ₂ of the backward pump light is preferablyset to 975 nm or 985 nm.

According to the above embodiments of the present invention, thewavelength λ₁ of the forward pump light and the wavelength λ₂ of thebackward pump light fall within the same pump band, where λ₁ ≠λ₂. Thepump band is determined so that a doped optical fiber of a doped fiberamplifier has a gain band which includes the wavelength of signal lightto be amplified. For example, in the case that an optical fiber is dopedwith erbium for amplifying signal light falling within a 1.55 μm band,the pump band may be, for example, a 0.82 μm band, a 0.98 μm band or a1.48 μm band. Preferably, the 0.82 μm band is defined by wavelengthsbetween 0.80 μm and 0.84 μm, the 0.98 μm band is defined by wavelengthsbetween 0.96 μm and 1.00 μm, and the 1.48 μm band is defined bywavelengths between 1.46 μm and 1.50 μm. However, the present inventionis not intended to be limited to these precise pump bands, and theranges of the bands can easily be changed. For example, another, moreprecise, preferably range for the 0.98 μm band is between 0.965 μm and0.995 μm.

Optical repeaters are used to provide long distance opticalcommunication. Thus, optical repeaters are often laid underneath theocean to provide optical communication between continents. Such opticalrepeaters typically include a doped fiber amplifier. Therefore, it ispreferably for a doped fiber amplifier used in an optical repeater toprovide redundant functions, since it is difficult to repair or maintainan optical repeater laid underneath the ocean.

A doped fiber amplifier which uses bidirectional pumping, such as thedoped fiber amplifiers illustrated in FIGS. 1 and 6, can provide theneeded redundancy since one of the pump light sources will still amplifysignal light propagating through the optical fiber when the other pumplight source has failed. In this case, by setting a noise figure and again provided by the wavelength λ₁ of the forward pump lightsubstantially equal to a noise figure and a gain provided by thewavelength λ₂ of the backward pump light, a constant noise figure orgain tilt can be maintained even when one of the two pump lights isreduced in power to cause a change in power balance.

For example, as illustrated in FIG. 7, gain curve 35 and noise figurecurve 33 have shapes which are symmetrical with respect to λ_(minNF) sothat λ_(minNF) is substantially equal to (λ₁ +λ₂)/2. Specifically, oneof λ₁ and λ₂ is preferable equal to 975 nm or 985 nm, and the other ofλ₁ and λ₂ is preferable equal to the other of 975 nm or 985 nm.

FIG. 8 is a graph illustrating gain tilt of a doped fiber amplifierwhich uses an erbium doped fiber. More specifically, FIG. 8 showsspectra of a WDM signal light amplified by such a doped fiber amplifier.The WDM signal light includes four signal lights, or channels, havingwavelengths of 1548 nm, 1551 nm, 1554 nm, and 1557 nm, respectively.Each of the channels of the WDM signal light are input to the dopedfiber amplifier with the same input power (-35 dBm/ch). In FIG. 8, thevertical axis represents output power (dBm) and the horizontal axisrepresents wavelength (nm).

The spectrum "A" illustrated in FIG. 8 corresponds to the case where thepower of pump light is relatively large. In this case, a negative gaintilt occurs. That is, the differential of gain with respect towavelength is negative (dG/dλ<0).

The spectrum "C" illustrated in FIG. 8 corresponds to the case where thepower of pump light is relatively small. In this case, a positive gaintilt is obtained (dG/dλ>0).

The spectrum "B" illustrated in FIG. 8 corresponds to the case where thepower of pump light is optimum such that no gain tilt occurs. In thiscase, the differential of gain with respect to wavelength is 0(dG/dλ=0).

Each spectrum shown in FIG. 8 has a shape in which four sharp spectracorresponding to the four channels of the WDM signal light aresuperimposed on a gentle spectrum of amplified spontaneous emission(ASE). The wavelength range where ASE is generated so as to obtain sucha gain is referred to as a "gain band" of the doped fiber amplifier.

In a doped fiber amplifier, gain characteristics of signals arereflected on a spectrum of ASE. Accordingly, the gain tilt of a dopedfiber amplifier can be detected by monitoring ASE. Therefore, based on amonitored ASE, the gain tilt can be feedback-controlled so as to becomeflat or constant. This concept will now be described in more detailbelow.

FIG. 9 is a diagram illustrating a doped fiber amplifier, according to afurther embodiment of the present invention. The doped fiber amplifierillustrated in FIG. 9 is similar to the doped fiber amplifierillustrated in FIG. 1, but includes a gain tilt control unit 37 whichmonitors ASE in doped fiber 2, determines a gain tilt from the monitoredASE and controls pump light to control the tilt gain.

More specifically, tilt gain control unit 37 includes an optical coupler32 connected to first end 2A of doped fiber 2 for extracting ASE fromfirst end 2A, a monitor 34 for receiving the ASE to detect a gain tiltin doped fiber 2, and a control circuit 36 for controlling at least oneof drive currents for laser diodes 12 and 18 so that the gain tiltdetected by monitor 34 becomes flat or constant.

Optical coupler 32 has ports 32A, 32B, 32C, and 32D. Port 32D ispreferably an angle cut fiber end, or is terminated by an antireflectioncoating, to reduce reflection. Almost all of the light supplied to port32A is output from port 320, and a portion of light supplied to port 32Cis output from port 32B. Port 32A is connected to an output port ofoptical isolator 24, and port 32C is connected to port 4A of opticalcoupler 4.

Gain tilt monitor 34 includes an optical coupler 38 (such as a 3-dBcoupler), optical band-pass filters 40 and 42, and photodetectors (PD)44 and 46. Photodetectors 44 and 46 are preferably photodiodes. Opticalcoupler 38 receives ASE output from port 32B of optical coupler 32 andbranches the ASE into a first branched signal light and a secondbranched signal light. Optical band-pass filter 40 has a pass bandincluded in a gain band of doped fiber 2, for receiving the firstbranched light. Photodetector 44 converts the optical signal output fromoptical band-pass filter 40 into an electrical signal. Optical band-passfilter 42 has a pass band included in the gain band, but different fromthe pass band of optical band-pass filter 40, for receiving the secondbranched light. Photodetector 46 converts the optical signal output fromoptical band-pass filter 42 into an electrical signal.

Control circuit 36 controls a drive current of laser diode 12 and/orlaser diode 18 so that the ratio between output signals fromphotodetectors 44 and 46 becomes constant (for example, 1:1). Drivecircuits 16 (see FIG. 1) and 22 (see FIG. 1) are included in controlcircuit 36 illustrated in FIG. 9.

For example, in the gain band shown in FIG. 8, the center wavelength inthe pass band of optical band-pass filter 40 is set to 1540 nm, and thecenter wavelength of the pass band of optical band-pass filter 42 is setto 1560 nm. In this manner, the gain tilt can be monitored by detectingthe ratio between powers of the ASEs limited by the two pass bands.

A flat gain tilt, for example, can be obtained by performing feedbackcontrol such that the levels of electrical output signals fromphotodetectors 44 and 46 becomes constant. Thus, with a doped fiberamplifier as illustrated in FIG. 9, a stable gain and a constant gaintilt can be provided.

FIG. 10 a diagram illustrating control circuit 36, according to anembodiment of the present invention. Referring now to FIG. 10, in thecase that photodetectors 44 and 46 are photodiodes, photocurrentsflowing in the photodiodes are converted into voltage signals which aresupplied to input ports of a divider 48.

An output level of divider 48 corresponding to the ratio between inputvoltage signals is compared with a reference voltage V_(REF) in anoperational amplifier 50, and laser diode 12 (or 18) is driven accordingto a difference between the output level and the reference voltageV_(REF). A power transistor 52 generates a drive current.

The above-described feedback control for providing a constant gain tiltis especially effective in the case that a noise figure and a gainprovided by the wavelength of forward pump light are substantially equalto a noise figure and a gain provided by the wavelength of backward pumplight. That is, according to the above embodiments of the presentinvention, in the case that one of the two pump light sources isdeteriorated, a change in gain tilt can be prevented.

In the above embodiments of the present invention, the wavelength of thesignal light preferable falls within a 1.55 μm band, and erbium is adopant of the doped fiber. In this case, the pump band is set topreferably a 0.98 μm band, so as to obtain a low noise figure and a highpumping efficiency. Alternatively, the pump band may be set to a 1.48 μmband, so as to obtain a doped fiber amplifier having high output power.However, the present invention is not intended to be limited to signallight within a specific band, pump light within a specific band, or theuse of a specific rare earth element as a dopant. Instead, variousdifferent rare earth elements, amplification bands, and pump bands canbe selected based on the specific requirements of the communicationsystem.

According to the above embodiments of the present invention, a dopedfiber amplifier is provided which uses bidirectional pumping, butreduces instability of gain caused by the bidirectional pumping.

Various optical components described herein are "operatively connected"to each other. The term "operatively connected" refers to opticalcomponents being directly connected together by fiber connection,spatially connected using a collimated beam, or connected throughanother optical component such as an optical filter.

Although a few preferred embodiments of the present invention have beenshown and described, it would be appreciated by those skilled in the artthat changes may be made in these embodiments without departing from theprinciples and spirit of the invention, the scope of which is defined inthe claims and their equivalents.

What is claimed is:
 1. An apparatus for amplifying a signal light,comprising:an optical fiber having first and second ends, the signallight propagating through the optical fiber from the first end to thesecond end; a first light source providing pump light which propagatesin the optical fiber from the first end to the second end and is at afirst wavelength; and a second light source providing pump light whichpropagates in the optical fiber from the second end to the first end andis at a second wavelength which is different from the first wavelength,the pump light provided by the first and second light sources causingthe signal light to be amplified as the signal light propagates throughthe optical fiber, wherein the pump lights produced by the first andsecond light sources are within the same pump band, and the firstwavelength is substantially equal to a wavelength which provides aminimum noise figure in the pump band.
 2. An apparatus as in claim 1,wherein the first light source comprises:a laser diode producing lightat the first wavelength; and a reflection type optical device whichnarrows the spectrum of the light produced by the laser diode andoutputs the narrowed spectrum light as the pump light provided by thefirst light source.
 3. An apparatus as in claim 2, wherein the secondlight source comprises:a laser diode producing light at the secondwavelength; and a reflection type optical device which narrows thespectrum of the light produced by the laser diode and outputs thenarrowed spectrum light as the pump light provided by the second lightsource.
 4. An apparatus as in claim 2, wherein the reflection typeoptical device is a grating fiber.
 5. An apparatus as in claim 3,wherein the reflection type optical devices are grating fibers.
 6. Anapparatus as in claim 1, wherein the first light source comprises alaser diode operating in a single mode in a wavelength band having thefirst wavelength as a center wavelength.
 7. An apparatus as in claim 6,wherein the second light source comprises a laser diode operating in asingle mode in a wavelength band having the second wavelength as acenter wavelength.
 8. An apparatus as in claim 1, wherein the opticalfiber is doped with erbium, the signal light is within a 1.55 μm band,and the pump lights produced by the first and second light sources arewithin a 0.98 μm band.
 9. An apparatus as in claim 8, wherein the firstwavelength is substantially equal to a wavelength which provides aminimum noise figure in the 0.98 μm band.
 10. An apparatus as in claim8, wherein the first wavelength is substantially equal to 980 nm, andthe second wavelength falls within a range of 965 nm to 995 nm.
 11. Anapparatus as in claim 1, wherein the second wavelength is substantiallyequal to a wavelength which provides a maximum gain in the pump band.12. An apparatus as in claim 11, wherein the second wavelength issubstantially equal to either 975 nm or 985 nm.
 13. An apparatus as inclaim 8, wherein the first wavelength provides a noise figure and a gainwhich is substantially equal to a noise figure and a gain provided bythe second wavelength.
 14. An apparatus as in claim 1, wherein thewavelength which provides the minimum noise figure in the pump band issubstantially equal to one-half of the sum of the first and secondwavelengths.
 15. An apparatus as in claim 1, wherein the firstwavelength is substantially equal to one of the group consisting of 975nm and 985 nm, and the second wavelength is substantially equal to theother of the group consisting of 975 nm and 985 nm.
 16. An apparatus asin claim 1, wherein the first and second wavelengths are different by atleast 5 nm.
 17. An apparatus as in claim 1, wherein at least one of thegroup consisting of the first and second light sources comprise adistributed-feedback (DFB) laser diode.
 18. An apparatus as in claim 1,wherein the first and second light sources each comprise adistributed-feedback (DFB) laser diode.
 19. An apparatus for amplifyinga signal light, comprising:an optical fiber, the signal lightpropagating through the optical fiber in a forward direction; a firstlight source providing pump light to the optical fiber at a firstwavelength and in the forward direction; and a second light sourceproviding pump light to the optical fiber at a second wavelength and ina backward direction opposite the first direction, wherein the firstwavelength is different from the second wavelength and the pump lightsprovided by the first and second light sources together causebi-directional pumping to amplify the signal light as the signal lightpropagates through the optical fiber, wherein the pump lights producedby the first and second light sources are within the same pump band, andthe first wavelength is substantially equal to a wavelength whichprovides a minimum noise figure in the pump band.
 20. A method foramplifying a signal light propagating through an optical fiber havingfirst and second ends, the method comprising the steps of:propagatingthe signal light through the optical fiber from the first end to thesecond end; propagating first pump light at a first wavelength in theoptical fiber from the first end to the second end so that the firstpump light causes the signal light to be amplified as the signal lightpropagates through the optical fiber; and propagating second pump lightat a second wavelength in the optical fiber from the second end to thefirst end so that the second pump light causes the signal light to beamplified as the signal light propagates through the optical fiber, thefirst wavelength being a different wavelength than the secondwavelength, wherein the first and second pump lights are within the samepump band, and the first wavelength is substantially equal to awavelength which provides a minimum noise figure in the pump band.
 21. Amethod as in claim 20, wherein the step of propagating first pump lightcomprises the steps of:producing light at the first wavelength; andnarrowing the spectrum of the produced light and providing the narrowedspectrum light as the first pump light.
 22. A method as in claim 20,wherein the step of propagating second pump light comprises the stepsof:producing light at the second wavelength; and narrowing the spectrumof the produced light and providing the narrowed spectrum light as thesecond pump light.
 23. A method as in claim 20, wherein the opticalfiber is doped with erbium, the signal light is within a 1.55 μm band,and the first and second pump lights are within a 0.98 μm band.
 24. Amethod as in claim 20, wherein the second wavelength is substantiallyequal to a wavelength which provides a maximum gain in the pump band.25. An apparatus for amplifying a signal light, comprising:an opticalfiber having first and second ends, the signal light propagating throughthe optical fiber from the first end to the second end; a first lightsource providing pump light which propagates in the optical fiber fromthe first end to the second end and is at a first wavelength; and asecond light source providing pump light which propagates in the opticalfiber from the second end to the first end and is at a second wavelengthwhich is different from the first wavelength, the pump light provided bythe first and second light sources causing the signal light to beamplified as the signal light propagates through the optical fiber,whereinthe pump lights produced by the first and second light sourcesare within the same pump band, the first wavelength is substantiallyequal to a wavelength which provides a minimum noise figure in the pumpband, and the second wavelength is substantially equal to a wavelengthwhich provides a maximum gain in the pump band.
 26. A method foramplifying a signal light propagating through an optical fiber havingfirst and second ends, the method comprising the steps of:propagatingthe signal light through the optical fiber from the first end to thesecond end; propagating first pump light at a first wavelength in theoptical fiber from the first end to the second end so that the firstpump light causes the signal light to be amplified as the signal lightpropagates through the optical fiber; and propagating second pump lightat a second wavelength in the optical fiber from the second end to thefirst end so that the second pump light causes the signal light to beamplified as the signal light propagates through the optical fiber, thefirst wavelength being a different wavelength than the secondwavelength, whereinthe first and second pump lights are within the samepump band, the first wavelength is substantially equal to a wavelengthwhich provides a minimum noise figure in the pump band, and the secondwavelength is substantially equal to a wavelength which provides amaximum gain in the pump band.